Published figures by group
Investigating strangeness enhancement in jet and medium via $φ$(1020) production in p$-$Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV
Figure 3a
- Fig. Group : Investigating strangeness enhancement in jet and medium via $φ$(1020) production in p$-$Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV
- PWG : PWG-LF (Light Flavour Spectra)
- System: p-Pb
- Energy: 5.02 TeV
Figure 3b
- Fig. Group : Investigating strangeness enhancement in jet and medium via $φ$(1020) production in p$-$Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV
- PWG : PWG-LF (Light Flavour Spectra)
- System: p-Pb
- Energy: 5.02 TeV
Figure 3c
- Fig. Group : Investigating strangeness enhancement in jet and medium via $φ$(1020) production in p$-$Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV
- PWG : PWG-LF (Light Flavour Spectra)
- System: p-Pb
- Energy: 5.02 TeV
Figure 3d
- Fig. Group : Investigating strangeness enhancement in jet and medium via $φ$(1020) production in p$-$Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV
- PWG : PWG-LF (Light Flavour Spectra)
- System: p-Pb
- Energy: 5.02 TeV
Figure 3e
- Fig. Group : Investigating strangeness enhancement in jet and medium via $φ$(1020) production in p$-$Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV
- PWG : PWG-LF (Light Flavour Spectra)
- System: p-Pb
- Energy: 5.02 TeV
Figure 3f
- Fig. Group : Investigating strangeness enhancement in jet and medium via $φ$(1020) production in p$-$Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV
- PWG : PWG-LF (Light Flavour Spectra)
- System: p-Pb
- Energy: 5.02 TeV
Figure 4a
- Fig. Group : Investigating strangeness enhancement in jet and medium via $φ$(1020) production in p$-$Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV
- PWG : PWG-LF (Light Flavour Spectra)
- System: p-Pb
- Energy: 5.02 TeV
Figure 4b
- Fig. Group : Investigating strangeness enhancement in jet and medium via $φ$(1020) production in p$-$Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV
- PWG : PWG-LF (Light Flavour Spectra)
- System: p-Pb
- Energy: 5.02 TeV
Figure 5a
- Fig. Group : Investigating strangeness enhancement in jet and medium via $φ$(1020) production in p$-$Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV
- PWG : PWG-LF (Light Flavour Spectra)
- System: p-Pb
- Energy: 5.02 TeV
Figure 5b
- Fig. Group : Investigating strangeness enhancement in jet and medium via $φ$(1020) production in p$-$Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV
- PWG : PWG-LF (Light Flavour Spectra)
- System: p-Pb
- Energy: 5.02 TeV
Charm fragmentation fractions and ${\rm c\overline{c}}$ cross section in p$-$Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV
Figure 1a
- Fig. Group : Charm fragmentation fractions and ${\rm c\overline{c}}$ cross section in p$-$Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: p-Pb
- Energy: 5.02 TeV
Figure 1b
- Fig. Group : Charm fragmentation fractions and ${\rm c\overline{c}}$ cross section in p$-$Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: p-Pb
- Energy: 5.02 TeV
Figure 2
- Fig. Group : Charm fragmentation fractions and ${\rm c\overline{c}}$ cross section in p$-$Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV
- PWG : PWG-HF (Heavy Flavour)
- System: p-Pb
- Energy: 5.02 TeV
Measurement of ${}_Λ^{3}\mathrm{H}$ production in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV
Figure 1
- Fig. Group : Measurement of ${}_Λ^{3}\mathrm{H}$ production in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV
- PWG : PWG-LF (Light Flavour Spectra)
- System: Pb-Pb
- Energy: 5.02 TeV
Figure 2
- Fig. Group : Measurement of ${}_Λ^{3}\mathrm{H}$ production in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV
- PWG : PWG-LF (Light Flavour Spectra)
- System: Pb-Pb
- Energy: 5.02 TeV
Figure 3
- Fig. Group : Measurement of ${}_Λ^{3}\mathrm{H}$ production in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV
- PWG : PWG-LF (Light Flavour Spectra)
- System: Pb-Pb
- Energy: 5.02 TeV
Figure 4
- Fig. Group : Measurement of ${}_Λ^{3}\mathrm{H}$ production in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV
- PWG : PWG-LF (Light Flavour Spectra)
- System: Pb-Pb
- Energy: 5.02 TeV
Rapidity dependence of antideuteron coalescence in pp collisions at $\sqrt{s}$ = 13 TeV with ALICE
Figure 1a
- Fig. Group : Rapidity dependence of antideuteron coalescence in pp collisions at $\sqrt{s}$ = 13 TeV with ALICE
- PWG : PWG-LF (Light Flavour Spectra)
- System: p-p
- Energy: 13 TeV
Figure 1b
- Fig. Group : Rapidity dependence of antideuteron coalescence in pp collisions at $\sqrt{s}$ = 13 TeV with ALICE
- PWG : PWG-LF (Light Flavour Spectra)
- System: p-p
- Energy: 13 TeV
Figure 2a
- Fig. Group : Rapidity dependence of antideuteron coalescence in pp collisions at $\sqrt{s}$ = 13 TeV with ALICE
- PWG : PWG-LF (Light Flavour Spectra)
- System: p-p
- Energy: 13 TeV
Figure 2b
- Fig. Group : Rapidity dependence of antideuteron coalescence in pp collisions at $\sqrt{s}$ = 13 TeV with ALICE
- PWG : PWG-LF (Light Flavour Spectra)
- System: p-p
- Energy: 13 TeV
Figure 3a
- Fig. Group : Rapidity dependence of antideuteron coalescence in pp collisions at $\sqrt{s}$ = 13 TeV with ALICE
- PWG : PWG-LF (Light Flavour Spectra)
- System: p-p
- Energy: 13 TeV
Figure 3b
- Fig. Group : Rapidity dependence of antideuteron coalescence in pp collisions at $\sqrt{s}$ = 13 TeV with ALICE
- PWG : PWG-LF (Light Flavour Spectra)
- System: p-p
- Energy: 13 TeV
Figure 4a
- Fig. Group : Rapidity dependence of antideuteron coalescence in pp collisions at $\sqrt{s}$ = 13 TeV with ALICE
- PWG : PWG-LF (Light Flavour Spectra)
- System: p-p
- Energy: 13 TeV
Figure 4b
- Fig. Group : Rapidity dependence of antideuteron coalescence in pp collisions at $\sqrt{s}$ = 13 TeV with ALICE
- PWG : PWG-LF (Light Flavour Spectra)
- System: p-p
- Energy: 13 TeV